Final Magnetic Moment0.000 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingNM |
Formation Energy / Atom-4.332 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.181 eVThe energy of decomposition of this material into the set of most stable materials at this chemical composition, in eV/atom. Stability is tested against all potential chemical combinations that result in the material's composition. For example, a Co2O3 structure would be tested for decomposition against other Co2O3 structures, against Co and O2 mixtures, and against CoO and O2 mixtures. |
Density6.46 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLaF3 |
Band Gap4.919 eVIn general, band gaps computed with common exchange-correlation functionals such as the LDA and GGA are severely underestimated. Typically the disagreement is reported to be ~50% in the literature. Some internal testing by the Materials Project supports these statements; typically, we find that band gaps are underestimated by ~40%. We additionally find that several known insulators are predicted to be metallic. |
Hermann MauguinFm3m [225] |
Hall-F 4 2 3 |
Point Groupm3m |
Crystal Systemcubic |
Calculated powder diffraction pattern; note that peak spacings may be affected due to inaccuracies in calculated cell volume, which is typically overestimated on average by 3% (+/- 6%)
Select an element to display a spectrum averaged over all sites of that element in the structure.
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Download spectra for every symmetrically equivalent absorption site in the structure.
Download FEFF Input parameters.
substrate material | substrate orientation | film orientation | MCIA† [Å2] |
---|---|---|---|
LaAlO3 (mp-2920) | <1 0 1> | <1 1 1> | 238.2 |
LaAlO3 (mp-2920) | <0 0 1> | <1 1 1> | 178.6 |
AlN (mp-661) | <0 0 1> | <1 1 1> | 59.5 |
AlN (mp-661) | <1 0 1> | <1 1 0> | 243.1 |
AlN (mp-661) | <1 1 1> | <1 1 0> | 194.5 |
GaAs (mp-2534) | <1 0 0> | <1 0 0> | 34.4 |
GaAs (mp-2534) | <1 1 1> | <1 1 1> | 59.5 |
GaN (mp-804) | <0 0 1> | <1 1 0> | 243.1 |
GaN (mp-804) | <1 0 1> | <1 0 0> | 171.9 |
AlN (mp-661) | <1 1 0> | <1 1 0> | 291.7 |
CeO2 (mp-20194) | <1 0 0> | <1 0 0> | 275.0 |
GaAs (mp-2534) | <1 1 0> | <1 1 0> | 48.6 |
BaF2 (mp-1029) | <1 0 0> | <1 0 0> | 309.4 |
GaN (mp-804) | <1 0 0> | <1 1 0> | 340.3 |
GaN (mp-804) | <1 1 1> | <1 0 0> | 275.0 |
SiO2 (mp-6930) | <1 0 1> | <1 1 0> | 145.9 |
DyScO3 (mp-31120) | <0 0 1> | <1 1 0> | 97.2 |
DyScO3 (mp-31120) | <1 1 0> | <1 0 0> | 309.4 |
InAs (mp-20305) | <1 0 0> | <1 0 0> | 309.4 |
ZnSe (mp-1190) | <1 1 1> | <1 1 1> | 59.5 |
KCl (mp-23193) | <1 0 0> | <1 0 0> | 171.9 |
DyScO3 (mp-31120) | <1 0 0> | <1 0 0> | 137.5 |
DyScO3 (mp-31120) | <1 0 1> | <1 0 0> | 171.9 |
ZnSe (mp-1190) | <1 0 0> | <1 0 0> | 34.4 |
ZnSe (mp-1190) | <1 1 0> | <1 1 0> | 48.6 |
KTaO3 (mp-3614) | <1 0 0> | <1 0 0> | 275.0 |
KTaO3 (mp-3614) | <1 1 0> | <1 0 0> | 240.6 |
KTaO3 (mp-3614) | <1 1 1> | <1 0 0> | 171.9 |
CdS (mp-672) | <1 0 0> | <1 0 0> | 171.9 |
LiF (mp-1138) | <1 0 0> | <1 0 0> | 34.4 |
YVO4 (mp-19133) | <0 0 1> | <1 0 0> | 275.0 |
YVO4 (mp-19133) | <1 0 0> | <1 1 1> | 178.6 |
TePb (mp-19717) | <1 0 0> | <1 0 0> | 171.9 |
CdS (mp-672) | <0 0 1> | <1 0 0> | 240.6 |
CdS (mp-672) | <1 0 1> | <1 1 0> | 340.3 |
CdS (mp-672) | <1 1 0> | <1 1 1> | 297.7 |
LiF (mp-1138) | <1 1 0> | <1 1 0> | 48.6 |
LiF (mp-1138) | <1 1 1> | <1 0 0> | 171.9 |
Te2W (mp-22693) | <0 1 1> | <1 1 0> | 291.7 |
Ag (mp-124) | <1 0 0> | <1 0 0> | 34.4 |
Ag (mp-124) | <1 1 0> | <1 1 0> | 48.6 |
Ag (mp-124) | <1 1 1> | <1 0 0> | 240.6 |
Bi2Te3 (mp-34202) | <0 0 1> | <1 1 0> | 340.3 |
GaSe (mp-1943) | <0 0 1> | <1 1 1> | 238.2 |
BN (mp-984) | <0 0 1> | <1 1 0> | 291.7 |
BN (mp-984) | <1 0 0> | <1 0 0> | 309.4 |
BN (mp-984) | <1 1 0> | <1 1 0> | 340.3 |
BN (mp-984) | <1 1 1> | <1 1 1> | 238.2 |
LiNbO3 (mp-3731) | <1 0 0> | <1 1 0> | 145.9 |
Bi2Se3 (mp-541837) | <0 0 1> | <1 1 1> | 59.5 |
Stiffness Tensor Cij (GPa) |
|||||
---|---|---|---|---|---|
72 | 58 | 58 | 0 | 0 | 0 |
58 | 72 | 58 | 0 | 0 | 0 |
58 | 58 | 72 | 0 | 0 | 0 |
0 | 0 | 0 | 3302 | 0 | 0 |
0 | 0 | 0 | 0 | 3302 | 0 |
0 | 0 | 0 | 0 | 0 | 3302 |
Compliance Tensor Sij (10-12Pa-1) |
|||||
---|---|---|---|---|---|
50.6 | -22.7 | -22.7 | 0 | 0 | 0 |
-22.7 | 50.6 | -22.7 | 0 | 0 | 0 |
-22.7 | -22.7 | 50.6 | 0 | 0 | 0 |
0 | 0 | 0 | 0.3 | 0 | 0 |
0 | 0 | 0 | 0 | 0.3 | 0 |
0 | 0 | 0 | 0 | 0 | 0.3 |
Shear Modulus GV1984 GPa |
Bulk Modulus KV63 GPa |
Shear Modulus GR17 GPa |
Bulk Modulus KR63 GPa |
Shear Modulus GVRH1000 GPa |
Bulk Modulus KVRH63 GPa |
Elastic Anisotropy578.17 |
Poisson's Ratio-0.76 |
material | dissimilarity | Ehull | # of elements |
---|---|---|---|
MnNi2Sn (mp-20440) | 0.0000 | 0.010 | 3 |
CuSnRh2 (mp-30595) | 0.0000 | 0.000 | 3 |
TiCuHg2 (mp-11882) | 0.0000 | 0.253 | 3 |
ZrCdCu2 (mp-11293) | 0.0000 | 0.000 | 3 |
LiAl2Pt (mp-30819) | 0.0000 | 0.000 | 3 |
LiMgSnPd (mp-7555) | 0.0000 | 0.000 | 4 |
LiMgSnAu (mp-7554) | 0.0000 | 0.088 | 4 |
VFeCoGe (mp-1063914) | 0.0000 | 0.000 | 4 |
LiMgSbPd (mp-10179) | 0.0000 | 0.096 | 4 |
LiMgSnPt (mp-11806) | 0.0000 | 0.000 | 4 |
NaIn (mp-20628) | 0.0000 | 0.000 | 2 |
SmMg3 (mp-30779) | 0.0000 | 0.065 | 2 |
AlCu3 (mp-12777) | 0.0000 | 0.025 | 2 |
LiZn (mp-1934) | 0.0000 | 0.000 | 2 |
CeCd3 (mp-2863) | 0.0000 | 0.000 | 2 |
Mg (mp-110) | 0.0000 | 0.022 | 1 |
He (mp-23158) | 0.0000 | 0.000 | 1 |
Mo (mp-129) | 0.0000 | 0.000 | 1 |
Pu (mp-107) | 0.0000 | 0.546 | 1 |
Tb (mp-11446) | 0.0000 | 0.148 | 1 |
Explore more synthesis descriptions for materials of composition LaF3.
Text computed by synthesisproject.org.
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: La F |
Final Energy/Atom-6.6319 eV |
Corrected Energy-27.9135 eV
Uncorrected energy = -26.5275 eV
Composition-based energy adjustment (-0.462 eV/atom x 3.0 atoms) = -1.3860 eV
Corrected energy = -27.9135 eV
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Displaying lattice parameters for primitive cell; note that calculated cell volumes are typically overestimated on average by 3% (+/- 6%). Note the primitive cell may appear less symmetric than the conventional cell representation (see "Structure Type" selector below the 3d structure)